Ori, Tetsuya (Koshigaya, JP)

Plaque It! Sponsored by: Flash of Genius

11/329138

06/27/2006

01/11/2006

Images are available in PDF form when logged in. To view PDFs, Login  or  Create Account (Free!)

View patents that cite this patent

Click for automatic bibliography generation

Fujinon Corporation (Saitama, JP)

359/557

359/740, 359/715, 359/684, 359/772, 359/686, 359/685, 359/774, 359/683

G02B15/14

359/554, 359/772, 359/686-687, 359/774, 359/715, 359/683-685, 359/557, 359/676, 359/740, 359/678

5677792	Zooming optical system	October, 1997	Hamano	359/557
6473231	Variable magnification optical system having image stabilizing function	October, 2002	Hamano et al.	359/557
6650475	Variable power optical system and image pick-up apparatus having the same	November, 2003	Hamano	359/557
6718132	Zoom lens, camera apparatus and portable information terminal apparatus	April, 2004	Nishina	359/684
6771432	Zoom lens, and electronic imaging system using the same	August, 2004	Mihara	359/687
6781755	Viewing optical system with an image-blur correcting optical system	August, 2004	Yoneyama	359/554
6999240	Zoom lens and video camera using it	February, 2006	Yamada et al.	359/683
20020024732	VARIABLE MAGNIFICATION OPTICAL SYSTEM HAVING IMAGE STABILIZING FUNCTION	February, 2002	Hamano et al.	359/557

JP2004151552	May, 2004
JP2004212737	July, 2004

Lester, Evelyn A.

Arnold International
Henry, Jon W.
Arnold, Bruce Y.

What is claimed is:

1. A zoom optical system with a vibration correction function comprising, arranged along an optical axis in order from the object side as follows: a first lens group having positive refractive power and that is stationary during zooming; a second lens group having negative refractive power and that moves along the optical axis during zooming; a third lens group having positive refractive power that includes a stop and that is stationary during zooming; and a fourth lens group having positive refractive power that moves along the optical axis during zooming; wherein said first lens group includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism for bending the optical axis, and at least one lens element having positive refractive power; and at least part of said third lens group is movable in a direction that intersects the optical axis in order to correct for blurring of an image due to vibration of the zoom optical system.

2. The zoom optical system of claim 1, wherein: said third lens group includes at least one lens element having positive refractive power and at least one lens element having negative refractive power; and at least one of said at least one lens element having positive refractive power of said third lens group or said at least one lens element having negative refractive power of said third lens group is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

3. The zoom optical system of claim 1, wherein said third lens group includes only a single lens element, and said single lens element is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

4. A zoom optical system with a vibration correction function comprising, arranged along an optical axis in order from the object side as follows: a first lens group having positive refractive power and that is stationary during zooming; a second lens group having negative refractive power and that moves along the optical axis during zooming; a third lens group having positive refractive power that includes a stop and that moves along the optical axis during zooming; and a fourth lens group that is stationary during zooming; wherein said first lens group includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism for bending the optical axis, and at least one lens element having positive refractive power; and at least part of said fourth lens group is movable in a direction that intersects the optical axis in order to correct for blurring of an image due to vibration of the zoom optical system.

5. The zoom optical system of claim 4, wherein: said fourth lens group includes at least one lens component formed by cementing together at least two lens elements and a separate single lens element that forms a lens component; and at least one of said one lens component and said separate single lens element is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

6. A zoom optical system with a vibration correction function comprising, arranged along an optical axis in order from the object side as follows: a first lens group having positive refractive power and that is stationary during zooming; a second lens group having negative refractive power and that moves along the optical axis during zooming; a third lens group having positive refractive power that includes a stop and that is stationary during zooming; a fourth lens group having positive refractive power that moves along the optical axis during zooming; and a fifth lens group that is stationary during zooming; wherein said first lens group includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism for bending the optical axis, and at least one lens element having positive refractive power; and at least part of said third lens group is movable in a direction that intersects the optical axis in order to correct for blurring of an image due to vibration of the zoom optical system.

7. The zoom optical system of claim 6, wherein: said third lens group includes at least one lens element having positive refractive power and at least one lens element having negative refractive power; and at least one of said at least one lens element having positive refractive power of said third lens group and said at least one lens element having negative refractive power of said third lens group is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

8. The zoom optical system of claim 6, wherein said third lens group includes only a single lens element, and said single lens element is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

9. A zoom optical system with a vibration correction function comprising, arranged along an optical axis in order from the object side as follows: a first lens group having positive refractive power and that is stationary during zooming; a second lens group having negative refractive power and that moves along the optical axis during zooming; a third lens group having positive refractive power that includes a stop and that is stationary during zooming; a fourth lens group having positive refractive power that moves along the optical axis during zooming; and a fifth lens group that does not move along the optical axis during zooming; wherein said first lens group includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism for bending the optical axis, and at least one lens element having positive refractive power; and at least part of said fifth lens group is movable in a direction that intersects the optical axis in order to correct for blurring of an image due to vibration of the zoom optical system.

10. The zoom optical system of claim 9, wherein: said fifth lens group includes at least one lens element having positive refractive power and at least one lens element having negative refractive power; and at least one of said at least one lens element having positive refractive power of said fifth lens group and said at least one lens element having negative refractive power of said fifth lens group is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

11. The zoom optical system of claim 9, wherein said fifth lens group includes only a single lens element, and said single lens element is movable in a direction that intersects the optical axis in order to correct for said blurring of an image due to vibration of the zoom optical system.

12. The zoom optical system of claim 1, wherein: said prism is between the most object side lens element of said first lens group having negative refractive power and the most object side lens element of said first lens group having positive refractive power; and the following condition is satisfied:
0.6<t_d/f_w<1.8 where t_d is the air equivalent optical conversion distance along the optical axis between said most object side lens element of said first lens group having negative refractive power and the said most object side lens element of said first lens group having positive refractive power; and f_w is the focal length of the entire zoom optical system at the wide-angle end.

13. The zoom optical system of claim 4, wherein: said prism is between the most object side lens element of said first lens group having negative refractive power and the most object side lens element of said first lens group having positive refractive power; and the following condition is satisfied:
0.6<t_d/f_w<1.8 where t_d is the air equivalent optical conversion distance along the optical axis between said most object side lens element of said first lens group having negative refractive power and the said most object side lens element of said first lens group having positive refractive power; and f_w is the focal length of the entire zoom optical system at the wide-angle end.

14. The zoom optical system of claim 6, wherein: said prism is between the most object side lens element of said first lens group having negative refractive power and the most object side lens element of said first lens group having positive refractive power; and the following condition is satisfied:
0.6<t_d/f_w<1.8 where t_d is the air equivalent optical conversion distance along the optical axis between said most object side lens element of said first lens group having negative refractive power and the said most object side lens element of said first lens group having positive refractive power; and f_w is the focal length of the entire zoom optical system at the wide-angle end.

15. The zoom optical system of claim 9, wherein: said prism is between the most object side lens element of said first lens group having negative refractive power and the most object side lens element of said first lens group having positive refractive power; and the following condition is satisfied:
0.6<t_d/f_w<1.8 where t_d is the air equivalent optical conversion distance along the optical axis between said most object side lens element of said first lens group having negative refractive power and the said most object side lens element of said first lens group having positive refractive power; and f_w is the focal length of the entire zoom optical system at the wide-angle end.

16. An imaging device including the zoom optical system of claim 1.

17. An imaging device including the zoom optical system of claim 4.

18. An imaging device including the zoom optical system of claim 6.

19. An imaging device including the zoom optical system of claim 9.

20. An imaging device including the zoom optical system of claim 12.

TECHNICAL FIELD OF THE INVENTION

The present invention relates to a zoom optical system with a vibration correction function and an imaging device using the zoom optical system that may be favorably implemented in imaging devices such as cellular telephones, portable computers, and similar devices.

BACKGROUND OF THE INVENTION

In recent years, cellular telephones, portable computers, and similar devices have included the capability of imaging picture information for viewing and recording with the use of an included imaging device. Furthermore, the imaging optical systems used in such imaging devices must be lightweight and compact for such applications in devices such as cellular telephones and portable computers. Additionally, technology has been developed in order to make such devices thinner in thickness by bending the optical axis of the optical systems by arranging prisms on the optical axis when the objective plane is in the thickness direction of the imaging device.

Moreover, there has also been a demand for higher level functions in the imaging optical systems in such imaging devices, and imaging optical systems having a zoom function have been proposed, for example, in Japanese Laid-Open Patent Application 2004-212737 and Japanese Laid-Open Patent Application 2004-151552.

When the imaging optical system is miniaturized, blurring occurs in the image being recorded when a slow shutter speed is used for recording because vibration caused by movement of a hand or hands holding the imaging device is transmitted to the imaging optical system. For this reason, high quality picture images frequently cannot be obtained due to image blurring.

A particular problem with imaging devices that include a zooming function is that blurring of images due to hand movement is especially significant at the telephoto end of the zoom range.

The technology described in Japanese Laid-Open Patent Application 2004-212737 and Japanese Laid-Open Patent Application 2004-151552 makes use of a first lens group having negative refractive power as a whole and including a prism, causing the diameter of diaphragms or stops used to increase in size and making the device thicker in the thickness direction.

The technology described in Japanese Laid-Open Patent Application 2004-212737 further has a limit to the miniaturization of the prism because the prism is provided at the object-most side of the first lens group.

BRIEF SUMMARY OF THE INVENTION

The present invention relates to a zoom optical system that provides favorable optical performance even when vibration due to hand movement or other causes occurs, with the zoom optical system including technology for making the zoom optical system thinner in the thickness direction by bending the optical axis. The present invention further relates to an imaging device using such a zoom optical system.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will become more fully understood from the detailed description given below and the accompanying drawings, which are given by way of illustration only and thus are not limitative of the present invention, wherein:

FIG. 1 shows a cross-sectional view of the zoom optical system of Embodiment 1 at the wide-angle end;

FIG. 2 shows a cross-sectional view of the zoom optical system of Embodiment 2-1 at the wide-angle end;

FIG. 3 shows a cross-sectional view of the zoom optical system of Embodiment 2-2 at the wide-angle end;

FIG. 4 shows a cross-sectional view of the zoom optical system of Embodiment 2-3 at the wide-angle end;

FIG. 5 shows a cross-sectional view of the zoom optical system of Embodiment 3-1 at the wide-angle end;

FIG. 6 shows a cross-sectional view of the zoom optical system of Embodiment 3-2 at the wide-angle end;

FIG. 7 shows a cross-sectional view of the zoom optical system of Embodiment 3-3 at the wide-angle end;

FIG. 8 shows a cross-sectional view of the zoom optical system of Embodiment 4 at the wide-angle end;

FIG. 9 shows a cross-sectional view of the zoom optical system of Embodiment 5 at the wide-angle end;

FIG. 10 shows a cross-sectional view of the zoom optical system of Embodiment 6-1 at the wide-angle end;

FIG. 11 shows a cross-sectional view of the zoom optical system of Embodiment 6-2 at the wide-angle end;

FIG. 12 shows a cross-sectional view of the zoom optical system of Embodiment 7-1 at the wide-angle end;

FIG. 13 shows a cross-sectional view of the zoom optical system of Embodiment 8-1 at the wide-angle end;

FIG. 14 shows a cross-sectional view of the zoom optical system of Embodiment 9-1 at the wide-angle end;

FIG. 15 shows a cross-sectional view of the zoom optical system of Embodiment 9-2 at the wide-angle end;

FIG. 16 shows a cross-sectional view of the zoom optical system of Embodiment 9-3 at the wide-angle end;

FIG. 17 shows a cross-sectional view of the zoom optical system of Embodiment 10-1 at the wide-angle end;

FIG. 18 shows a cross-sectional view of the zoom optical system of Embodiment 10-2 at the wide-angle end;

FIG. 19 shows a cross-sectional view of the zoom optical system of Embodiment 10-3 at the wide-angle end;

FIG. 20 shows a cross-sectional view of the zoom optical system of Embodiment 7-2 at the wide-angle end;

FIG. 21 shows a cross-sectional view of the zoom optical system of Embodiment 8-2 at the wide-angle end;

FIG. 22 shows a cross-sectional view of the zoom optical system of Embodiment 11-1 at the wide-angle end;

FIG. 23 shows a cross-sectional view of the zoom optical system of Embodiment 11-2 at the wide-angle end;

FIG. 24 shows a cross-sectional view of the zoom optical system of Embodiment 11-3 at the wide-angle end;

FIG. 25 shows a cross-sectional view of the zoom optical system of Embodiment 12-1 at the wide-angle end;

FIG. 26 shows a cross-sectional view of the zoom optical system of Embodiment 12-2 at the wide-angle end;

FIG. 27 shows a cross-sectional view of the zoom optical system of Embodiment 12-3 at the wide-angle end;

FIGS. 28A–28D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 1 at the wide-angle end, and

FIGS. 28E–28H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 1 at the telephoto end;

FIGS. 29A–29D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 2-1, 2-2, and 2-3 at the wide-angle end, and

FIGS. 29E–29H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 2-1, 2-2, and 2-3 at the telephoto end;

FIGS. 30A–30D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 3-1, 3-2, and 3-3 at the wide-angle end, and

FIGS. 30E–30H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 3-1, 3-2, and 3-3 at the telephoto end;

FIGS. 31A–31D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 4 at the wide-angle end, and

FIGS. 31E–31H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 4 at the telephoto end;

FIGS. 32A–32D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 5 at the wide-angle end, and

FIGS. 32E–32H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 5 at the telephoto end;

FIGS. 33A–33D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 6-1 and 6-2 at the wide-angle end, and

FIGS. 33E–33H the show spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 6-1 and 6-2 at the telephoto end;

FIGS. 34A–34D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 7-1 and 7-2 at the wide-angle end, and

FIGS. 34E–34H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 7-1 and 7-2 at the telephoto end;

FIGS. 35A–35D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 8-1 and 8-2 at the wide-angle end, and

FIGS. 35E–35H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 8-1 and 8-2 at the telephoto end;

FIGS. 36A–36D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 9-1, 9-2, and 9-3 at the wide-angle end, and

FIGS. 36E–36H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 9-1, 9-2, and 9-3 at the telephoto end;

FIGS. 37A–37D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 10-1, 10-2, and 10-3 at the wide-angle end, and

FIGS. 37E–37H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 10-1, 10-2, and 10-3 at the telephoto end;

FIGS. 38A–38D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 11-1, 11-2, and 11-3 at the wide-angle end, and

FIGS. 38E–38H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 11-1, 11-2, and 11-3 at the telephoto end; and

FIGS. 39A–39D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 12-1, 12-2, and 12-3 at the wide-angle end, and

FIGS. 39E–39H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiments 12-1, 12-2, and 12-3 at the telephoto end.

DETAILED DESCRIPTION

A brief general description of the zoom optical system with a vibration correction function of the present invention is given below. Specific embodiments of the zoom optical system will be described generally with references to various drawings. The embodiments described below are divided into four groups of embodiments.

FIGS. 1–8 show cross-sectional views of the zoom optical systems of the present invention that are constructed of four lens groups and include a vibration correction function to prevent blurring of an image being viewed or recorded due to vibration of the zoom optical system. The vibration correction function is achieved by moving at least a part of the third lens group from the object side in a direction that intersects the optical axis of the zoom optical system. FIGS. 1–8 relate to the first group of embodiments of the present invention.

FIGS. 9–11 also show cross-sectional views of the zoom optical systems of the present invention that are constructed of four lens groups and include a vibration correction function to prevent blurring of an image being viewed or recorded due to vibration of the zoom optical system. However, in this case, the vibration correction function is achieved by moving at least a part of the fourth lens group from the object side in a direction that intersects the optical axis of the zoom optical system. FIGS. 9–11 relate to the second group of embodiments of the present invention.

FIGS. 12–19 show cross-sectional views of the zoom optical systems that are constructed of five lens groups and include a vibration correction function to prevent blurring of an image being viewed or recorded due to vibration of the zoom optical system. The vibration correction function is achieved by moving at least a part of the third lens group from the object side in a direction that intersects the optical axis of the zoom optical system. FIGS. 12–19 relate to the third group of embodiments of the present invention.

FIGS. 20–27 also show cross-sectional views of the zoom optical systems of the present invention that are constructed of five lens groups and include a vibration correction function to prevent blurring of an image being viewed or recorded due to vibration of the zoom optical system. However, in this case, the vibration correction function is achieved by moving at least a part of the fifth lens group from the object side in a direction that intersects the optical axis of the zoom optical system. FIGS. 20–27 relate to the fourth group of embodiments of the present invention.

The zoom optical systems of the present inventions use lens groups that include lens elements and lens components. The term “lens group” is defined in terms of “lens elements” and “lens components” as explained herein. The term “lens element” is herein defined as a single transparent mass of refractive material having two opposed refracting surfaces that are oriented at least generally transverse to the optical axis of the zoom optical system. The term “lens component” is herein defined as (a) a single lens element spaced so far from any adjacent lens element that the spacing cannot be neglected in computing the optical image forming properties of the lens elements or (b) two or more lens elements that have their adjacent lens surfaces either in full overall contact or overall so close together that the spacings between adjacent lens surfaces of the different lens elements are so small that the spacings can be neglected in computing the optical image forming properties of the two or more lens elements. Thus, some lens elements may also be lens components. Therefore, the terms “lens element” and “lens component” should not be taken as mutually exclusive terms. In fact, the terms may frequently be used to describe a single lens element in accordance with part (a) above of the definition of a “lens component.” Alternatively, a lens component may frequently be made by cementing together two lens elements. The term “lens group” is herein defined as an assembly of one or more lens components in optical series and with no intervening lens components along an optical axis that during zooming is movable as a single unit relative to another lens component or other lens components.

The zoom optical system of the present invention will be further described with reference to FIG. 1 that shows Embodiment 1. An arrow at the lower left of FIG. 1 that points downward indicates the object side of the zoom optical system. In FIG. 1, lens elements are referenced by the letter L followed by a number denoting their order from the object side of the lens along the optical axis, from L1 to L10. Similarly, the radii of curvature of the optical surfaces are referenced by the letter R followed by a number denoting their order from the object side of the lens, from R1 to R23 in FIG. 1. The on-axis surface spacings along the optical axis of the various optical surfaces are referenced by the letter D followed by a number denoting their order from the object side of the lens, from D1 to D22 in FIG. 1. Additionally, in FIG. 1, solid line segments below the two lens groups, G2 and G4, indicate the movement of these two lens groups along the optical axis during zooming, with movement from the wide-angle end W to the telephoto end T of the zoom range being indicated by the downward direction in FIG. 1, and a double headed vertical arrow indicates the movement of the third lens group G3 in a direction that intersects the optical axis in order to correct for blurring of an image due to vibration of the zoom optical system. Furthermore, as shown in FIG. 1, a filter unit 2 that includes an infrared filter and/or similar structures, including a cover glass of a solid state image sensor, is provided adjacent the image plane 1 where an image is recorded. As shown in FIG. 1, lens group G4 is on the object side and adjacent the filter unit 2.

The first group of embodiments of the present invention are shown in FIGS. 1–8, which show Embodiments 1, 2-1, 2-2, 2-3, 3-1, 3-2, 3-3, and 4, respectively. These zoom optical systems with a vibration correction function include, arranged along an optical axis in order from the object side, a first lens group G1 having positive refractive power and that is stationary during zooming, a second lens group having negative refractive power and that moves along the optical axis during zooming, a third lens group G3 having positive refractive power that includes a stop or diaphragm 4 and that is stationary during zooming, and a fourth lens group G4 having positive refractive power that moves along the optical axis during zooming.

Furthermore, the straight line segment below the second lens group G2 and the curved line segment below the fourth lens group G4, indicate that the design is such that the fourth lens group G4 moves along the optical axis at a decreasing speed from the wide-angle end W to the telephoto end T when the second lens group G2 moves along the optical axis in a coordinated movement at a constant speed. In addition, the fourth lens group G4 also functions as the lens group for focusing.

In the zoom optical systems of the first group of embodiments of the present invention, the first lens group G1 includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism 3 for bending the optical axis, and at least one lens element having positive refractive power. Additionally, at least part of the third lens group G3 is movable in a direction that intersects the optical axis in order to correct for blurring of an image at the image plane 1 due to vibration of the zoom optical system. In particular, the third lens group includes only a single lens element or a lens element having positive refractive power and a lens element having negative refractive power, either or both of which may be movable in a direction that intersects the optical axis in order to correct for vibration of the zoom optical system.

The second group of embodiments of the present invention are shown in FIGS. 9–11, which show Embodiments 5, 6-1, and 6-2, respectively. These zoom optical systems with a vibration correction function include, arranged along an optical axis in order from the object side, a first lens group G1 having positive refractive power and that is stationary during zooming, a second lens group G2 having negative refractive power and that moves along the optical axis during zooming, a third lens group G3 having positive refractive power that includes a stop or diaphragm 4 and that moves along the optical axis during zooming, and a fourth lens group G4 that is stationary during zooming.

Furthermore, the straight line segment below the second lens group G2 and the curved line segment below the third lens group G3, indicate that the design is such that the third lens group G3 moves along the optical axis at a decreasing rate from the wide-angle end W to the telephoto end T when the second lens group G2 moves along the optical axis in a coordinated movement at a constant speed. In addition, the fourth lens group G4 also functions as the lens group for focusing.

In the zoom optical systems of the second group of embodiments of the present invention, the first lens group G1 includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism 3 for bending the optical axis, and at least one lens element having positive refractive power. Additionally, at least part of the fourth lens group G4 is movable in a direction that intersects the optical axis in order to correct for blurring of an image at the image plane 1 due to vibration of the zoom optical system. In particular, the fourth lens group G4 includes at least one lens component formed by cementing together at least two lens elements, and a single lens element that forms a lens component; and at least one of the cemented lens elements and the single lens element is movable in a direction that intersects the optical axis in order to correct for vibration of the zoom optical system.

The third group of embodiments of the present invention are shown in FIGS. 12–19, which show Embodiments 7-1, 8-1, 9-1, 9-2, 9-3, 10-1, 10-2, and 10-3, respectively. These zoom optical systems with a vibration correction function include, arranged along an optical axis in order from the object side, a first lens group G1 having positive refractive power and that is stationary during zooming, a second lens group G2 having negative refractive power and that moves along the optical axis during zooming, a third lens group G3 having positive refractive power that includes a stop or diaphragm 4 and that is stationary during zooming, a fourth lens group G4 having positive refractive power that moves along the optical axis during zooming, and a fifth lens group G5 that is stationary during zooming.

Furthermore, the straight line segment below the second lens group G2 and the curved line segment below the fourth lens group G4, indicate that the design is such that the fourth lens group G4 moves along the optical axis at a decreasing rate from the wide-angle end W to the telephoto end T while the second lens group G2 moves along the optical axis in a coordinated movement at a constant speed. In addition, the fourth lens group G4 also functions as the lens group for focusing.

In the zoom optical systems of the third group of embodiments of the present invention, the first lens group G1 includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism 3 for bending the optical axis, and at least one lens element having positive refractive power. Additionally, at least part of the third lens group G3 is movable in a direction that intersects the optical axis in order to correct for blurring of an image at the image plane 1 due to vibration of the zoom optical system. In particular, the third lens group includes only a single lens element or a lens element having positive refractive power and a lens element having negative refractive power, either or both of which may be movable in a direction that intersects the optical axis in order to correct for vibration of the zoom optical system.

The fourth group of embodiments of the present invention are shown in FIGS. 20–27, which show Embodiments 7-2, 8-2, 11-1, 11-2, 11-3, 12-1, 12-2, and 12-3, respectively. These zoom optical systems with a vibration correction function include, arranged along an optical axis in order from the object side, a first lens group G1 having positive refractive power and that is stationary during zooming, a second lens group G2 having negative refractive power and that moves along the optical axis during zooming, a third lens group G3 having positive refractive power that includes a stop or diaphragm 4 and that is stationary during zooming, a fourth lens group G4 having positive refractive power that moves along the optical axis during zooming, and a fifth lens group G5 that is stationary during zooming.

Furthermore, the straight line segment below the second lens group G2 and the curved line segment below the fourth lens group G4, indicate that the design is such that the fourth lens group G4 moves along the optical axis at a decreasing rate from the wide-angle end W to the telephoto end T while the second lens group G2 moves along the optical axis in a coordinated movement at a constant speed. In addition, the fourth lens group G4 also functions as the lens group for focusing.

In the zoom optical systems of the fourth group of embodiments of the present invention, the first lens group G1 includes, arranged along the optical axis in order from the object side, a lens element having negative refractive power, a prism 3 for bending the optical axis, and at least one lens element having positive refractive power. Additionally, at least part of the fifth lens group G5 is movable in a direction that intersects the optical axis in order to correct for blurring of an image at the image plane 1 due to vibration of the zoom optical system. In particular, the fifth lens group G5 includes only a single lens element or a lens element having positive refractive power and a lens element having negative refractive power, either or both of which may be movable in a direction that intersects the optical axis in order to correct for vibration of the zoom optical system.

All embodiments of all four groups of embodiments of the present invention described above, and described further below, satisfy the following condition:
0.6<t_d/f_w <1.8 Condition (1)
where

t_d is the air equivalent optical conversion distance along the optical axis between the most object side lens element of said first lens group having negative refractive power and the most object side lens element of said first lens group having positive refractive power; and

f_w is the focal length of the entire zoom optical system at the wide-angle end.

The air equivalent optical conversion distance td is calculated in order to take into account the index of refraction of the prism 3 varying from that of air according to the following equation:
t_d=D2+D4+(1/N 3)·D3
where

D2 is the distance, providing an air space, along the optical axis between the lens element L1 having negative refractive power provided at the object most side of the zoom optical system and the prism within the first lens group G1,

D3 is the distance along the optical axis of the prism 3 between the entrance and exit faces of the prism 3,

D4 is the distance, providing an air space, between the lens element of the first lens group G1 having positive refractive power provided nearest the object side of the zoom optical system and the prism within the first lens group G1, and

N3 is the refractive index of the prism 3 within the first lens group G1.

Satisfying Condition (1) above helps achieve miniaturization of the zoom optical system without light rays being excessively shielded from passing through the prism 3 to the image plane 1.

If the lower limit of Condition (1) is not satisfied there is insufficient space for a prism 3 of an appropriate size that appropriately shields and passes light rays to be provided between the lens elements having negative and positive refractive powers. If the upper limit of Condition (1) is not satisfied, the total length of the zoom optical system becomes too long. Furthermore, as the outer diameter of the lens element having negative refractive power within the first lens group G1 becomes larger, miniaturization of the zoom optical system becomes more difficult.

Additionally, in order to improve imaging and reduce aberrations, some of the surfaces of the lens elements in embodiments of the present invention are aspheric. The lens surfaces that are aspheric are defined using the following Equation (A):
Z=[(Y²/R)/{1+(1< i>−K·Y²/R²)^1/2}]+Σ(A_i·Yⁱ) Equation (A)
where

• • Z is the length (in mm) of a line drawn from a point on the aspheric lens surface at a distance Y from the optical axis to the tangential plane of the aspheric surface vertex,
  • R is the radius of curvature (in mm) of the aspheric lens surface on the optical axis,
  • Y is the distance (in mm) from the optical axis,
  • K is the eccentricity, and
  • A_i is the ith aspheric coefficient, and the summation extends over i.

In embodiments of the invention disclosed below, only aspheric coefficients A₃–A₁₂ are ever non-zero and sometimes some of these aspheric coefficients are also zero.

Embodiments of the zoom optical system of the present invention will now be individually described with reference to the drawings.

EMBODIMENT 1

FIG. 1 shows a cross-sectional view of the zoom optical system of Embodiment 1 at the wide-angle end. The zoom optical system of Embodiment 1 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 includes a stop or diaphragm 4 and a lens element having positive refractive power (i.e., the seventh lens element L7) that prevents blurring of an image formed at the image plane 1 by movement of this lens element L7 having positive refractive power in a direction that intersects the optical axis in order to correct for blurring of the image being recorded or viewed due to vibration of the zoom optical system.

As shown in FIG. 1, the first lens group G1 includes, arranged along the optical axis in order from the object side, a first lens element L1 having negative refractive power and a meniscus shape with its convex surface on the object side, a right-angle prism 3 that bends the optical axis, a biconvex second lens element L2, and a third lens element L3 having positive refractive power and a meniscus shape with a convex surface on the object side. The second lens group G2 includes, arranged along the optical axis in order from the object side, a biconcave fourth lens element L4, a biconcave fifth lens element L5, and a sixth lens element L6 having positive refractive power and a meniscus shape with its convex surface on the object side. The third lens group G3 includes, arranged along the optical axis in order from the object side, a stop or diaphragm 4 and a biconvex seventh lens element L7. The fourth lens group G4, includes, arranged along the optical axis in order from the object side, an eight lens element L8 having negative refractive power and a meniscus shape with its convex surface on the object side, a biconvex ninth lens element L9 and a tenth lens element L10 having negative refractive power with a convex surface on the image side.

In addition, the fifth lens element L5 and the sixth lens element L6 are cemented together at adjoining lens surfaces, as are also the eighth lens element L8 and the ninth lens element L9.

Also, in Embodiment 1, the filter unit 2 includes an infrared filter and/or similar structures, including a cover glass for a solid state image sensor, provided between the fourth lens group G4 and the image plane 1. An imaging device is represented in FIG. 1 by the combination of lens groups G1–G4, filter unit 2 and image plane 1, which is located where an image sensor can receive an image.

In the zoom optical system of Embodiment 1, the luminous flux that enters along the optical axis from the object side forms an image at the image formation position on the image plane 1, where a solid state image sensor (such as a CCD image sensor) is situated. Furthermore, the vibration correction function is activated when vibrations or movements, such as hand movements of the zoom optical system that may cause blurring of an image, occur. Such blurring of an image is corrected by moving the seventh lens element L7 that forms the third lens group G3 in a direction that intersects the optical axis.

Table 1 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface on the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N_d and the Abbe number ν_d (at the d-line) of each optical component for Embodiment 1, except that the on-axis surface spacings that vary with zooming are listed in Table 3 below. Listed in the bottom portion of Table 1 are the focal length f (in mm) and the f-number F_NO at the wide-angle and telephoto ends, and the maximum field angle 2ω at the wide-angle end and the telephoto end for Embodiment 1. Tables similar to those for Embodiment 1 below will be used later to describe the other embodiments of the present invention.

1.834810.10< td>1.72916< td>52.4∞ (stop)< td>18.9< td>64.2

TABLE 1
#	R	D	Nd	νd
1	29.0148	0.85	1.92286	20.9
2	13.0772	3.04
3	∞	11.00	42.7
4	∞
5	22.3889	3.12	54.7
6	−33.842 2	0.10
7	19.5591	2. 04	1.72916	54.7
8	3 4.3361	D8(variable)
9	−20.6119	0.65	1.77250	49.6
10	7.1771	1.20
11	−18.0172	0.61	1.51742
12	6.6697	1.77	1.84666	23.8
13	36.3807	D13(variable)
14	0.50
15*	8.4868	1.70	1.50842	56.4
16*	−49.7302	D16(variable)
17	8.2163	0.84	1.92286
18	5.0000	2.95	1.48749	70.2
19	−15.1 293	2.63
20*	−22.3944	1.10	1.56865	58.6
21*< /td>	−1077530.8	D21(variable)
22	∞	1.00	1.51680
23	∞
	f = 6.35–17.95	FNO = 3.63–3.92	2ω = 63.0°–22.2°

The lens surfaces with a * to the right of the surface number in Table 1 are aspheric lens surfaces, and the aspheric surface shapes of these lens surfaces are expressed by Equation (A) above.

Table 2 below lists the values of the constant K and the aspheric coefficients A₄, A₆, A₈, and A₁₀ in Equation (A) above for each of the aspheric lens surfaces of Table 1. Aspheric coefficients that are not present in Table 2 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base 10. For example, “1.0E-2” represents the number 1.0×10⁻².

TABLE 2
#	K	A4	A6	A8	A10< /sub>
15	0.8096721	6.6954749E -5	2.9300223E-6	7.4788973E-7	−5 .0481388E-9
16	1.0034934	3. 7323860E-4	9.4279759E-6	2.2432608E-7	1.1208807E-8
20	1.0707124	1.0623578E-4	−4.7518657E-6	1.5313145 E-7	9.5552489E-9
21	0.56 27926	4.1474356E-4	−1.1474039E-5	4 .8270807E-7	−1.8943477E-8

In the zoom optical system of Embodiment 1, lens groups G2 and G4 move to vary the on-axis surface spacings of the various the optical elements along the optical axis during zooming between the wide-angle end W and the telephoto end T of the zoom range. Therefore, the values of the on-axis surface spacings D₈, D₁₃, D₁₆, and D₂₁ vary. Table 3 below lists the value of the on-axis surface spacing D₈ between the lens surface on the extreme image side of the first lens group G1 and the lens surface of the object-most side of the second lens group G2, the on-axis surface spacing D₁₃ between the lens surface on the extreme image side of the second lens group G2 and the stop or diaphragm 4, the on-axis surface spacing D₁₆ between the lens surface of the extreme image side of the third lens group G3 and the lens surface of the object-most side of the fourth lens group G4, and the on-axis surface spacing D₂₁ between the lens surface of the extreme image side of the fourth lens group G4 and the object side surface of the filter unit 2, at the wide-angle end (focal length f equals 6.35 mm) and the telephoto end (focal length f equals 17.95 mm) in the zoom optical system of Embodiment 1 with the zoom optical system focused at infinity.

2.07

TABLE 3
Focal Length f (mm)	D8	D13	D< sub>16	D21
6.35	1.00	9.41	4.87	6.92
17.95	8.34	2.39	9.40

Additionally, the zoom optical system of Embodiment 1 satisfies Condition (1) with a value of t_d/f_w equal to 1.44.

FIGS. 28A–28D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 1 at the wide-angle end, and FIGS. 28E–28H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical of Embodiment 1 at the telephoto end. In FIGS. 28A and 28E, the spherical aberration (in mm) is shown for the wavelengths 587.6 nm (the d-line and indicated by a solid line), 460 nm (indicated by a dashed line), and 615 nm (indicated by a double dashed line), and the f-number is shown. In the remaining figures, ω is the half-field angle. In FIGS. 28B and 28F, the astigmatism (in mm) is shown for both the sagittal image surface S and the tangential image surface T and is measured at 587.6 nm (the d-line). In FIGS. 28C and 28G, distortion (in percent) is measured at 587.6 nm (the d-line). In FIGS. 28D and 28H, the lateral color (in μm) is shown for the wavelengths 460 nm and 615 nm relative to 587.6 nm (the d-line). Similar figures will be described with reference to the other embodiments of the present invention below.

As is evident from FIGS. 28A–28H, the zoom optical system of Embodiment 1 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 2-1

FIG. 2 shows a cross-sectional view of the zoom optical system of Embodiment 2-1 at the wide-angle end. The zoom optical system of Embodiment 2-1 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 prevents blurring of an image at the image plane 1 that would otherwise occur due to vibration of the zoom optical system by moving, in a direction that intersects the optical axis, the seventh lens element L7 having positive refractive power and the eighth lens element L8 having negative refractive power that are included in the third lens group G3.

As shown in FIG. 2, the first lens group G1 includes, arranged along the optical axis in order from the object side, a first lens element L1 having negative refractive power and a meniscus shape with its convex surface on the object side, a right-angle prism 3 that bends the optical axis, a biconvex second lens element L2, and a third lens element L3 having positive refractive power and a meniscus shape with its convex surface on the object side. The second lens group G2 includes, arranged along the optical axis in order from the object side, a biconcave fourth lens element L4, a biconcave fifth lens element L5, and a sixth lens element L6 having positive refractive power and a meniscus shape with its convex surface on the object side. The third lens group G3 includes, arranged along the optical axis in order from the object side, a stop or diaphragm 4, a biconvex seventh lens element L7, and an eighth lens element L8 having negative refractive power and a meniscus shape with its convex surface on the object side. The fourth lens group G4, includes, arranged along the optical axis in order from the object side, a ninth lens element L9 having negative refractive power and a meniscus shape with its convex surface on the object side, a biconvex tenth lens element L10 and an eleventh lens element L11 having negative refractive power and a meniscus shape with its convex surface on the image side.

In addition, the fifth lens element L5 and the sixth lens element L6 are cemented together at adjoining lens surfaces, as are also the ninth lens element L9 and the tenth lens element L10.

Also, in Embodiment 2-1, the filter unit 2 includes an infrared filter and/or similar structures, including a cover glass for a solid state image sensor, provided between the fourth lens group G4 and the image plane 1.

In the zoom optical system of Embodiment 2-1, the luminous flux that enters along the optical axis from the object side forms an image at the image formation position on the image plane 1, where a solid state image sensor (such as a CCD image sensor) is situated. Furthermore, the vibration correction function is activated when vibrations or movements, such as hand movements of the zoom optical system that may cause blurring of an image, occur. Such blurring of an image is corrected by moving the seventh lens element L7 and the eight lens element L8 that form the third lens group G3 in a direction that intersects the optical axis.

Specific data regarding the zoom optical system of Embodiment 2-1 are shown below in Tables 4-6. These tables are equally descriptive of Embodiments 2-2 and 2-3 that will be described after Embodiment 2-1.

Table 4 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface on the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N_d and the Abbe number ν_d (at the d-line) of each optical component for Embodiment 2-1, except that the on-axis surface spacings that vary with zooming are listed in Table 6 below. Listed in the bottom portion of Table 4 are the focal length f (in mm) and the f-number F_NO at the wide-angle and telephoto ends, and the maximum field angle 2ω at the wide-angle end and the telephoto end for Embodiment 2-1.

1.834810.10< td>1.72916< td>64.2∞ (stop)< tr>

TABLE 4
#	R	D	Nd	νd
1	31.7235	0.85	1.92286	20.9
2	12.8611	2.91
3	∞	11.00	42.7
4	∞
5	23.8003	3.13	54.7
6	−29.408 4	0.10
7	19.1389	2. 04	1.75500	54.7
8	3 4.2845	D8(variable)
9	−20.2147	0.65	1.75600	52.3
10	8.0477	1.20
11	−18.0172	0.61	1.51680
12	7.1392	1.75	1.84666	23.8
13	29.7317	D13(variable)
14	0.50
15*	7.6152	1.85	1.50842	56.4
16*	−20.0005	0.33
17	1 54.8902	0.60	1.84666	23.8
18	29.0224	D18(variable)
19	7.4389	0.61	1.922 86	18.9
20	5.0000	2 .95	1.48749	70.2
21	−15.5250	2.63
22*	−10. 9787	1.10	1.56865	58.6
23*	−50.1705	D23(variable)< /td>
24	∞	1.00	1.51680	64.2
25	∞
	f = 6.34–17.92	FNO = 3.60–3.86	2ω = 63.0°–22.0°

The lens surfaces with a * to the right of the surface number in Table 4 are aspheric lens surfaces, and the aspheric surface shapes of these lens surfaces are expressed by Equation (A) above.

Table 5 below lists the values of the constant K and the aspheric coefficients A₄, A₆, A₈, and A₁₀ in Equation (A) above for each of the aspheric lens surfaces of Table 4. Aspheric coefficients that are not present in Table 5 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base 10. For example, “1.0E-2” represents the number 1.0×10⁻².

TABLE 5
#	K	A4	A6	A8	A10< /sub>
15	0.7353000	−1.34158 98E-4	4.4553715E-6	7.6092782E-7	� ��5.0394055E-9
16	1.0087282	2.6884682E-4	1.1342275E-5	1.7017848E- 7	1.1177968E-8
22	1.1111 256	−1.8831251E-4	−7.4900491E-6	1.8100336E-7	9.1690095E-9
23	0.5622224	2.7492996E-4	−8.8154434E -6	5.0751243E-7	−1.9077591E-8

In the zoom optical system of Embodiment 2-1, lens groups G2 and G4 move to vary the on-axis surface spacings of the various optical elements along the optical axis during zooming between the wide-angle end W and the telephoto end T of the zoom range. Therefore, the values of the on-axis surface spacings D₈, D₁₃, D₁₈, and D₂₃ vary. Table 6 below lists the value of the on-axis surface spacing D₈ between the lens surface on the extreme image side of the first lens group G1 and the lens surface of the object-most side of the second lens group G2, the on-axis surface spacing D₁₃ between the lens surface on the extreme image side of the second lens group G2 and the stop or diaphragm 4, the on-axis surface spacing D₁₈ between the lens surface of the extreme image side of the third lens group G3 and the lens surface of the object-most side of the fourth lens group G4, and the on-axis surface spacing D₂₃ between the lens surface of the extreme image side of the fourth lens group G4 and the object side surface of the filter unit 2, at the wide-angle end (focal length f equals 6.34 mm) and the telephoto end (focal length f equals 17.92 mm) in the zoom optical system of Embodiment 2-1 with the zoom optical system focused at infinity.

2.07

TABLE 6
Focal Length f (mm)	D8	D13	D< sub>18	D23
6.34	1.00	9.49	4.45	6.16
17.92	8.42	2.39	8.22

Additionally, the zoom optical system of Embodiment 2-1 satisfies Condition (1) with a value of t_d/f_w equal to 1.42.

FIGS. 29A–29D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 2-1, as well as Embodiments 2-2 and 2-3, at the wide-angle end, and FIGS. 29E–29H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 2-1, as well as Embodiments 2-2 and 2-3, at the telephoto end. In FIGS. 29A and 29E, the spherical aberration (in mm) is shown for the wavelengths 587.6 nm (the d-line and indicated by a solid line), 460 nm (indicated by a dashed line), and 615 nm (indicated by a double dashed line), and the f-number is shown. In the remaining figures, ω is the half-field angle. In FIGS. 29B and 29F, the astigmatism (in mm) is shown for both the sagittal image surface S and the tangential image surface T and is measured at 587.6 nm (the d-line). In FIGS. 29C and 29G, distortion (in percent) is measured at 587.6 nm (the d-line). In FIGS. 29D and 29H, the lateral color (in μm) is shown for the wavelengths 460 nm and 615 nm relative to 587.6 nm (the d-line).

As is evident from FIGS. 29A–29H, the zoom optical system of Embodiment 2-1 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 2-2

FIG. 3 shows a cross-sectional view of the zoom optical system of Embodiment 2-2 at the wide-angle end. The zoom optical system of Embodiment 2-2 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 prevents blurring of an image at the image plane 1 that would otherwise occur due to vibration of the zoom optical system by moving, in a direction that intersects the optical axis, only the seventh lens element L7 having positive refractive power in the third lens group G3.

The zoom optical system of Embodiment 2-2 is nearly the same as Embodiment 2-1 above, the only difference being that unlike Embodiment 2-1, in this embodiment the eighth lens element L8 does not move in a direction that intersects the optical axis for vibration correction but rather remains stationary on the optical axis and only the seventh lens element L7 moves for vibration correction.

However, the lens and other optical element data of Tables 4–6 above of Embodiment 2-1 also describe Embodiment 2-2. Accordingly, the various aberrations, including the spherical aberration, astigmatism, distortion, and lateral color, of Embodiment 2-2 for the wide-angle and telephoto ends are the same as those shown in FIGS. 29A–29H.

Additionally, therefore, the zoom optical system of Embodiment 2-2 satisfies Condition (1) with a value of t_d/f_w equal to 1.42, the same value as Embodiment 2-1.

Furthermore, as is evident from FIGS. 29A–29H, the zoom optical system of Embodiment 2-2 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 2-3

FIG. 4 shows a cross-sectional view of the zoom optical system of Embodiment 2-3 at the wide-angle end. The zoom optical system of Embodiment 2-3 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 prevents blurring of the image at the image plane 1 that would otherwise occur due to vibration of the zoom optical system by moving, in a direction that intersects the optical axis, only the eighth lens element L8 having negative refractive power in the third lens group G3.

The zoom optical system of Embodiment 2-3 is nearly the same as Embodiment 2-1 above, the only difference being that, unlike Embodiment 2-1, in this embodiment the seventh lens element L7 does not move in a direction that intersects the optical axis for vibration correction but rather remains stationary on the optical axis and only the eighth lens element L8 moves for vibration correction.

However, the lens and other optical element data of Tables 4–6 above of Embodiment 2-1 also describe Embodiment 2-3. Accordingly, the various aberrations, including the spherical aberration, astigmatism, distortion, and lateral color of Embodiment 2-3 at the wide-angle and telephoto ends are the same as those shown in FIGS. 29A–20H.

Additionally, therefore, the zoom optical system of Embodiment 2-3 satisfies Condition (1) with a value of t_d/f_w equal to 1.42, the same value as Embodiment 2-1.

Furthermore, as is evident from FIGS. 29A–29H, the zoom optical system of Embodiment 2-3 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 3-1

FIG. 5 shows a cross-sectional view of the zoom optical system of Embodiment 3-1 at the wide-angle end. The zoom optical system of Embodiment 3-1 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 includes a lens element having positive refractive power (i.e., the sixth lens element L6) and a lens element having negative refractive power (i.e., the seventh lens element L7) that prevent blurring of an image formed at the image plane 1 by movement of these lens elements L6 and L7 in a direction that intersects the optical axis in order to correct for blurring of the image being recorded or viewed due to vibration of the zoom optical system.

As shown in FIG. 5, the first lens group G1 includes, arranged along the optical axis in order from the object side, a first lens element L1 having negative refractive power and a meniscus shape with its convex surface on the object side, a right-angle prism 3 that bends the optical axis, and a biconvex second lens element L2. The second lens group G2 includes, arranged along the optical axis in order from the object side, a biconcave third lens element L3, a biconcave fourth lens element L4, and a fifth lens element L5 having positive refractive power and a meniscus shape with its convex surface on the object side. The third lens group G3 includes, arranged along the optical axis in order from the object side, a stop or diaphragm 4, a biconvex sixth lens element L6, and a seventh lens element L7 having negative refractive power and a meniscus shape with its convex surface on the object side. The fourth lens group G4 includes, arranged along the optical axis in order from the object side, an eighth lens element L8 having negative refractive power and a meniscus shape with its convex surface on the object side, a biconvex ninth lens element L9, and a tenth lens element L10 having negative refractive power and a meniscus shape with its convex surface on the image side.

In addition, the fourth lens element L4 and the fifth lens element L5 are cemented together at adjoining lens surfaces, as are also the eighth lens element L8 and the ninth lens element L9.

Also, in Embodiment 3-1, the filter unit 2 includes an infrared filter and/or similar structures, including a cover glass for a solid state image sensor, provided between the fourth lens group G4 and the image plane 1.

In the zoom optical system of Embodiment 3-1, the luminous flux that enters along the optical axis from the object side forms an image at the image formation position on the image plane 1, where a solid state image sensor (such as a CCD image sensor) is situated. Furthermore, the vibration correction function is activated when vibrations or movements, such as hand movements of the zoom optical system that may cause blurring of an image, occur. Such blurring of an image is corrected by moving the sixth lens element L6 and the seventh lens element L7 that form the third lens group G3 in a direction that intersects the optical axis.

Specific data regarding the zoom optical system of Embodiment 3-1 are shown below in Tables 7–9. These tables are equally descriptive of Embodiments 3-2 and 3-3 that will be described after Embodiment 3-1.

Table 7 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface on the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N_d and the Abbe number ν_d (at the d-line) of each optical component for Embodiment 3-1, except that the on-axis surface spacings that vary with zooming are listed in Table 9 below. Listed in the bottom portion of Table 7 are the focal length f (in mm) and the f-number F_NO at the wide-angle and telephoto ends, and the maximum field angle 2ω at the wide-angle end and the telephoto end for Embodiment 3-1.

1.00

	TABLE 7
	#	R	D	Nd	νd
	1	46.9285	0.82< /td>	1.92286	20.9
	2	15.0000	2.20
	3	∞	10.3	1.83481	42.7
	4	∞	0.10
	5*	15 .0413	3.26	1.69350	53.2
	6*	−22.7747	D6 (variable)
	7	−22 .7142	0.60	1.75500	52.3
	8	7.5266	1.29
	9	−18.1072	0.61	1.51742	52.4
	10	6.9346	1 .83	1.84666	23.8
	11	33.3034	D11 (variable)
	12	∞ (stop)	0.50
	13*	6.4465	1.93	1.50842	56.4
	14*	−30.4906	0.30
< td>15	13.9329	0.60	1.84666	2 3.8
	16	8.5245	D16 (variable)
	17	6.9674	0.65	1.92286	18.9
	18	5.0000	2.79	1.48749	70.2
	19	−20.8484	2.61
	20*	−15.4088	1.10	1.56865	58.6
	21*	� ��11944.2800	D21 (variable)
	22	∞	1.51680	64.2
	23	∞
f = 6.35–17.95 FNO = 3.60–3.91 2ω = 63.2°–21.8°

The lens surfaces with a * to the right of the surface number in Table 7 are aspheric lens surfaces, and the aspheric surface shapes of these lens surfaces are expressed by Equation (A) above.

Table 8 below lists the values of the constant K and the aspheric coefficients A₃–A₁₀ in Equation (A) above for each of the aspheric lens surfaces of Table 7. Aspheric coefficients that are not present in Table 8 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base 10. For example, “1.0E-2” represents the number 1.0×10⁻².

< td>A₄< td>6

TABLE 8
#	K	A3	A5	A6	A7
5	0.9704877	2.67762 90E−4	−1.0690933E−4	6.2047760E−6	6.6378182E−7	−1.8924453E−8
1.0007739	2.8341350E−4	−2.0 219496E−5	−1.3818341E−7	2.0669726E−6	−5.3975569E−8
13	0.599 9317	0	−2.0141608E−4	0	1 .4908244E−6	0
14	1.006247 7	0	2.0930730E−4	0	6.36582 02E−6	0
20	1.0686721	0	−5.0558470E−4	0	−1.28293 37E−5	0
21	0.5591829	0	2.6374215E−4	0	−4.1889959E −6	0
	#	A8	A< sub>9	A10
	5	−2.2807156E−9	−1.0642299E−9	−1.3582263E−10
	6	1.6890434E−8	−2.8092697E� ��9	2.1808485E−10
	13	5.5903571E−7	0	−6.1280469E−9
	14	2.4545834E−7	0	1. 0759209E−8
	20	2.4311622E−8	0	9.2006557E−9
	21	6.9622172E−7	0	−1.8357838E−8

In the zoom optical system of Embodiment 3-1, lens groups G2 and G4 move to vary the on-axis surface spacings of various optical elements along the optical axis during zooming between the wide-angle end W and the telephoto end T of the zoom range. Therefore, the values of the on-axis surface spacings D₆, D₁₁, D₁₆, and D₂₁ vary. Table 9 below lists the value of the on-axis surface spacing D₆ between the lens surface on the extreme image side of the first lens group G1 and the lens surface of the object-most side of the second lens group G2, the on-axis surface spacing D₁₁ between the lens surface on the extreme image side of the second lens group G2 and the stop or diaphragm 4, the on-axis surface spacing D₁₆ between the lens surface of the extreme image side of the third lens group G3 and the lens surface of the object-most side of the fourth lens group G4, and the on-axis surface spacing D₂₁ between the lens surface of the extreme image side of the fourth lens group G4 and the object side surface of the filter unit 2, at the wide-angle end (focal length f equals 6.35 mm) and the telephoto end (focal length f equals 17.95 mm) in the zoom optical system of Embodiment 3-1 with the zoom optical system focused at infinity.

< td>2.45

TABLE 9
Focal Length f (mm)	D6	D11	D< sub>16	D21
6.35	1.00	10.01	4.53	6.48
17.95	8.55	2.37	8.63

Additionally, the zoom optical system of Embodiment 3-1 satisfies Condition (1) with a value of t_d/f_w equal to 1.25.

FIGS. 30A–30D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 3-1, as well as of Embodiments 3-2 and 3-3, at the wide-angle end, and FIGS. 30E–30H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical of Embodiment 3-1, as well as of Embodiments 3-2 and 3-3, at the telephoto end. In FIGS. 30A and 30E, the spherical aberration (in mm) is shown for the wavelengths 587.6 nm (the d-line and indicated by a solid line), 460 nm (indicated by a dashed line), and 615 nm (indicated by a double dashed line), and the f-number is shown. In the remaining figures, ω is the half-field angle. In FIGS. 30B and 30F, the astigmatism (in mm) is shown for both the sagittal image surface S and the tangential image surface T and is measured at 587.6 nm (the d-line). In FIGS. 30C and 30G, distortion (in percent) is measured at 587.6 nm (the d-line). In FIGS. 30D and 30H, the lateral color (in μm) is shown for the wavelengths 460 nm and 615 nm relative to 587.6 nm (the d-line).

As is evident from FIGS. 30A–30H, the zoom optical system of Embodiment 3-1 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 3-2

FIG. 6 shows a cross-sectional view of the zoom optical system of Embodiment 3-2 at the wide-angle end. The zoom optical system of Embodiment 3-2 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 prevents blurring of an image at the image plane 1 that would otherwise occur due to vibration of the zoom optical system by moving, in a direction that intersects the optical axis, only the sixth lens element L6 having positive refractive power in the third lens group G3.

The zoom optical system of Embodiment 3-2 is nearly the same as Embodiment 3-1 above, the only difference being that, unlike Embodiment 3-1, in this embodiment the seventh lens element L7 does not move in a direction that intersects the optical axis for vibration correction but rather remains stationary on the optical axis and only the sixth lens element L6 moves for vibration correction.

However, the lens and other optical element data of Tables 7–9 above of Embodiment 3-1 also describe Embodiment 3-2. Accordingly, the various aberrations, including the spherical aberration, astigmatism, distortion, and lateral color, of Embodiment 3-2 for the wide-angle and telephoto ends are the same as those shown in FIGS. 30A–30H.

Additionally, therefore, the zoom optical system of Embodiment 3-2 satisfies Condition (1) with a value of t_d/f_w equal to 1.25, the same value as Embodiment 3-1.

Furthermore, as is evident from FIGS. 30A–30H, the zoom optical system of Embodiment 3-2 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 3-3

FIG. 7 shows a cross-sectional view of the zoom optical system of Embodiment 3-3 at the wide-angle end. The zoom optical system of Embodiment 3-3 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 prevents blurring of an image at the image plane 1 that would otherwise occur due to vibration of the zoom optical system by moving, in a direction that intersects the optical axis, only the seventh lens element L7 having negative refractive power in the third lens group G3.

The zoom optical system of Embodiment 3-3 is nearly the same as Embodiment 3-1 above, the only difference being that unlike Embodiment 3-1 the sixth lens element L6 does not move in a direction that intersects the optical axis for vibration correction but rather remains stationary on the optical axis. That is, only the seventh lens element L7 moves for vibration correction.

However, the lens and other optical element data of Tables 7–9 above of Embodiment 3-1 also describe Embodiment 3-3. Accordingly, the various aberrations, including the spherical aberration, astigmatism, distortion, and lateral color, of Embodiment 3-3 at the wide-angle and telephoto ends are the same as those shown in FIGS. 30A–30H.

Additionally, therefore, the zoom optical system of Embodiment 3-3 satisfies Condition (1) with a value of t_d/f_w equal to 1.25, the same value as Embodiment 3-1.

Furthermore, as is evident from FIGS. 30A–30H, the zoom optical system of Embodiment 3-3 is a high performance zoom optical system capable of favorably correcting aberrations.

EMBODIMENT 4

FIG. 8 shows a cross-sectional view of the zoom optical system of Embodiment 4 at the wide-angle end. The zoom optical system of Embodiment 4 has a four lens group construction, and the third lens group G3 provides the vibration correction function. In particular, the third lens group G3 includes a lens element having positive refractive power (i.e., the seventh lens element L7) that prevents blurring of an image formed at the image plane 1 by movement of this lens element L7 having positive refractive power in a direction that intersects the optical axis in order to correct for blurring of the image being recorded or viewed due to vibration of the zoom optical system, and also includes the stop or diaphragm 4.

As shown in FIG. 8, the first lens group G1 includes, arranged along the optical axis in order from the object side, a first lens element L1 having negative refractive power and a meniscus shape with its convex surface on the object side, a right-angle prism 3 that bends the optical axis, a plano-convex second lens element L2, and a biconvex third lens element L3. The second lens group G2 includes, arranged along the optical axis in order from the object side, a fourth lens element L4 having negative refractive power and a meniscus shape with a convex surface on the object side, a biconcave fifth lens element L5, and a biconvex sixth lens element L6. The third lens group G3 includes, arranged along the optical axis in order from the object side, a biconvex seventh lens element L7 and the stop or diaphragm 4. The fourth lens group G4 includes, arranged along the optical axis in order from the object side, a biconvex eight lens element L8, a biconcave ninth lens element L9, and a tenth lens element L10 having positive refractive power and a meniscus shape with its convex surface on the object side.

In addition, the fifth lens element L5 and the sixth lens element L6 are cemented together at adjoining lens surfaces, as are also the eighth lens element L8 and the ninth lens element L9.

Also, in Embodiment 4, the filter unit 2 includes an infrared filter and/or similar structures, including a cover glass for a solid state image sensor, provided between the fourth lens group G4 and the image plane 1.

In the zoom optical system of Embodiment 4, the luminous flux that enters along the optical axis from the object side forms an image at the image formation position on the image plane 1, where a solid state image sensor (such as a CCD image sensor) is situated. Furthermore, the vibration correction function is activated when vibrations or movements, such as hand movements of the zoom optical system that may cause blurring of an image, occur. Such blurring of an image is corrected by moving the seventh lens element L7 that forms the third lens group G3 in a direction that intersects the optical axis.

Table 10 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of each surface on the optical axis, the on-axis surface spacing D (in mm), as well as the refractive index N_d and the Abbe number ν_d (at the d-line) of each optical component for Embodiment 4, except that the on-axis surface spacings that vary with zooming are listed in Table 12 below. Listed in the bottom portion of Table 10 are the focal length f (in mm) and the f-number F_NO at the wide-angle and telephoto ends, and the maximum field angle 2ω at the wide-angle end and the telephoto end for Embodiment 4.

< td/>< td>1.588091.922860.83

	TABLE 10
	#	R	D	Nd	νd
	1	54.8917	0.76< /td>	1.92286	20.9
	2	10.9715	2.09
	3	∞	8.10	1.83481	42.7
4	∞	0.05
	5	∞	1.25	1.75520	27.5
	6	−37.2448	0.10
	7*	14.0779	2.35	60.4
	8*	−19.1783	D8 (variable)
	9	58.3809< /td>	0.58	1.72916	54.7
	10	8.3596	1.09
	11< /td>	−9.2871	0.60	1.80400	46.6< /td>
	12	12.9680	1.55	18.9
	13	−1 68.8569	D13 (variable)
	14*	8.6331	1.25	1.51007	56.2
15*	−76.0640	0.50
	16	∞ (stop)	D16 (variable)
	17	5.8907	2.01	1.83481	42.7
	18	−74.8060	0.59	1.84666	23.8
	19	4.5889	0.24
	20*	5.6911	1.60	1.51530	62.8
	21*	26.06 80	D21 (variable)
	22	∞	1.51680	64.2
	23	∞
f = 6.34–17.93 FNO = 3.59–4.27 2ω = 62.6°–22.0°

The lens surfaces with a * to the right of the surface number in Table 10 are aspheric lens surfaces, and the aspheric surface shapes of these lens surfaces are expressed by Equation (A) above.

Table 11 below lists the values of the constant K and the aspheric coefficients A₃–A₁₂ in Equation (A) above for each of the aspheric lens surfaces of Table 10. Aspheric coefficients that are not present in Table 11 are zero. An “E” in the data indicates that the number following the “E” is the exponent to the base 10. For example, “1.0E-2” represents the number 1.0×10⁻².

< td>A₄< td> 4.4513947E−4

TABLE 11
#	K	A3	A5	A6	A7	A8
7	0.9042386	2.45 20549E−4	−7.9692904E−5	−2.8018362E� �5	5.0025113E−6	9.0331766E−8	6.6795346E−8
8	0.9770572	−1.8004757E−4	6. 2236853E−6	4.8378460E−6	−6.4157530E− 8	3.0444581E−8
14	1.13 29410	0	6.8550321E−5	0	3.8417326E−6	0	2.0596064E−6< /td>
15	0.9987394	0	� ��3.6694963E−4	0	2.7410339E−5	0	−1.8018674E−6
20	1.7000254	2.4261209E−4	5.3720100E− 4	8.8773062E−6	3.0577261E−5	� ��2.3271041E−7	2.6163662E−6
21	1.0333767	−1.0035360E−4	2. 7951369E−3	−7.2485598E−5	7.3517201E− 5	−4.8998957E−7	1.0875630E−5
	#	A9	A< sub>10	A11	A12
	7	−6.6889889E−9	−1.4118112E−9	−3.7172727E−10	� ��2.5741176E−11
	8	−1.37767 70E−8	−2.5760713E−9	−1.0405539E−10	7.5729919E−12
	14	0	−1.0909457E−7	0	0
	15	0	9.3620748E− 8	0	0
	20	3.5827687E−11	7.2786675E−8	−5.1 735533E−11	1.6894719E−13
21	−1.0550646E−9	1.8032897E−7	−1.7358934E−10	−2.5370451E−11

In the zoom optical system of Embodiment 4, lens groups G2 and G4 move to vary the on-axis surface spacings of various optical elements along the optical axis during zooming between the wide-angle end W and the telephoto end T of the zoom range. Therefore, the values of the on-axis surface spacings D₈, D₁₃, D₁₆, and D₂₁ vary. Table 12 below lists the value of the on-axis surface spacing D₈ between the lens surface on the extreme image side of the first lens group G1 and the lens surface of the object-most side of the second lens group G2, the on-axis surface spacing D₁₃ between the lens surface on the extreme image side of the second lens group G2 and the lens surface on the object-most side of the third lens group G3, the on-axis surface spacing D₁₆ between the diaphragm or stop 4 and the lens surface of the object-most side of the fourth lens group G4, and the on-axis surface spacing D₂₁ between the tens surface of the extreme image side of the fourth lens group G4 and the object side surface of the filter unit 2, at the wide-angle end (focal length f equals 6.34 mm) and the telephoto end (focal length f equals 17.93 mm) in the zoom optical system of Embodiment 4 with the zoom optical system focused at infinity.

0.21

TABLE 12
Focal Length f (mm)	D8	D13	D< sub>16	D21
6.34	0.23	6.79	5.29	9.80
17.93	6.80	1.93	13.16

Additionally, the zoom optical system of Embodiment 4 satisfies Condition (1) with a value of t_d/f_w equal to 1.03.

FIGS. 31A–31D show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 4 at the wide-angle end, and FIGS. 31E–31H show the spherical aberration, astigmatism, distortion, and lateral color, respectively, of the zoom optical system of Embodiment 4 at the telephoto end. In FIGS. 31A and 31E, the spherical aberration (in mm) is shown for the wavelengths 587.6 nm (the d-line and indicated by a solid line), 460 nm (indicated by a dashed line), and 615 nm (indicated by a double dashed line), and the f-number is shown. In the remaining figures, ω is the half-field angle. In FIGS. 31B and 31F, the astigmatism (in mm) is shown for both the sagittal image surface S and the tangential image surface T and is measured at 587.6 nm (the d-line). In FIGS. 31C and 31G, distortion (in percent) is measured at 587.6 nm (the d-line). In FIGS. 31D and 31H, the lateral color (in μm) is shown for the wavelengths 460 nm and 615 nm relative to 587.6 nm (the d-line).

As is evident from FIGS. 31A–31H, the zoom optical system of Embodiment 4 is a high performance zoom optical system capable of favorably correcting aberrations.

The efficient operation of embodiments of the present invention described above that belong to the first group of embodiments of the present invention is explained below.

According to zoom optical systems belonging to the first group of embodiments of the present invention, because the third lens group G3 having positive refractive power is stationary during zooming, the exit angles of light rays to the imaging plane side can be reduced in the entire zooming range from the wide-angle end all the way to the telephoto end, and the change of exit angles of light rays when zooming can also be reduced. For this reason, these zoom optical systems are especially suitable for an imaging device using a solid state image sensor such as a CCD or similar device.

Furthermore, because the third lens group G3 that prevents vibration by moving in a direction to intersect the optical axis, is stationary during zooming, the construction of the lens frame of the third lens group G3 can be simplified. Furthermore, because the third lens group G3 is provided in the vicinity of the diaphragm or stop 4 (in fact, by including the diaphragm or stop 4 in the third lens group G3), the outer diameter of the lens elements of the third lens group G3 can be smaller, and therefore the lens frame can be smaller.

Additionally, when, as in Embodiments 1 and 4 above, the third lens group G3 is constructed as a single lens element having positive refractive power, the zoom optical system becomes particularly suitable for miniaturization. Furthermore, by arranging the construction of the third lens group G3 with only, arranged along the optical axis in order from the object side, the diaphragm or stop 4 and a lens element having positive refractive power, as in Embodiment 1 above, the change in the exit angle of light rays to the image plane side during zooming can be reduced. For this reason, this becomes especially suitable for an imaging device using a solid state image sensor such as a CCD or similar device.

Furthermore, when the third lens group G3 includes one lens element having positive refractive power and one lens element having negative refractive power, as in Embodiments 2-1, 2-2, 2-3, 3-1, 3-2, and 3-3 above, the axial chromatic aberration can be reduced, and the field curvature can also be reduced by having the Petzval sum be an appropriate value. In this case, miniaturization of the zooming optical system becomes possible by constructing the third lens group G3 of, arranged along the optical axis in order from the object side, the stop or diaphragm 4, a lens element having positive refractive power, and a lens element having negative refractive power.

Moreover, by preventing blurring of an image being recorded at the image plane 1 (which normally accompanies vibration of the zoom optical system) by moving all the lens elements of the third lens group G3 in a direction that intersects the optical axis, as in Embodiments 1, 2-1, 3-1, and 4, the change of the optical performance of the zoom optical system at the time of vibration correction can be minimized.

Furthermore, by preventing blurring of an image being recorded at the image plane 1, which normally accompanies vibration of the zoom optical system, by moving less than all of the lens elements of the third lens group G3 in the direction to intersect the optical axis, as in Embodiments 2-2, 2-3, 3-2 and 3-3, the weight of the lens elements that are moved in order to correct for vibration is reduced, and the load of the vibration correction mechanism can be reduced.

Furthermore, by preventing blurring of an image being recorded at the image plane 1, which normally accompanies vibration of the zoom optical system, by moving only the lens element having positive refractive power within the third lens group G3 in the direction to intersect the optical axis, as in Embodiments 1, 2-2 and 3-2, the degree of movement of an image on the image plane 1 at the time of vibration correction increases in comparison with the case of correcting vibration by moving the lens element having negative refractive power, thereby enabling vibration correction performance to be sufficient with a small degree of movement.

Furthermore, by preventing blurring of an image being recorded at the image plane 1, which normally accompanies vibration of the zoom optical system, by moving only the lens element having negative refractive power within the third lens group G3 in the direction to intersect the optical axis, as in Embodiments 2-3 and 3-3, the weight of the lens element that is moved at the time of vibration correction becomes smaller in comparison with the case of preventing vibration by moving a lens element having positive refractive power, thereby enabling the load of the